Camera Optical Lens

ABSTRACT

The present disclosure discloses a camera optical lens. The camera optical lens including, in an order from an object side to an image side, a first lens, a second lens having a negative refractive power, a third lens having a negative refractive power, a fourth lens, a fifth lens, and a sixth lens. The first lens is made of plastic material, the second lens is made of plastic material, the third lens is made of glass material, the fourth lens is made of plastic material, the fifth lens is made of plastic material, and the sixth lens is made of plastic material. The camera optical lens further satisfies specific conditions.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application claims the priority benefit of Chinese PatentApplications Ser. No. 201810065854.6 and Ser. No. 201810065396.6 filedon Jan. 23, 2018, the entire content of which is incorporated herein byreference.

FIELD OF THE PRESENT DISCLOSURE

The present disclosure relates to optical lens, in particular to acamera optical lens suitable for handheld devices such as smart phonesand digital cameras and imaging devices.

DESCRIPTION OF RELATED ART

With the emergence of smart phones in recent years, the demand forminiature camera lens is increasing day by day, but the photosensitivedevices of general camera lens are no other than Charge Coupled Device(CCD) or Complementary metal-Oxide Semiconductor Sensor (CMOS sensor),and as the progress of the semiconductor manufacturing technology makesthe pixel size of the photosensitive devices shrink, coupled with thecurrent development trend of electronic products being that theirfunctions should be better and their shape should be thin and small,miniature camera lens with good imaging quality therefor has become amainstream in the market. In order to obtain better imaging quality, thelens that is traditionally equipped in mobile phone cameras adopts athree-piece or four-piece lens structure. And, with the development oftechnology and the increase of the diverse demands of users, and underthis circumstances that the pixel area of photosensitive devices isshrinking steadily and the requirement of the system for the imagingquality is improving constantly, the five-piece, six-piece andseven-piece lens structure gradually appear in lens design. There is anurgent need for ultra-thin wide-angle camera lenses which have goodoptical characteristics and the chromatic aberration of which is fullycorrected.

BRIEF DESCRIPTION OF THE DRAWINGS

Many aspects of the exemplary embodiments can be better understood withreference to the following drawings. The components in the drawing arenot necessarily drawn to scale, the emphasis instead being placed toupon clearly illustrating the principles of the present disclosure.

FIG. 1 is a schematic diagram of a camera optical lens in accordancewith a first embodiment of the present invention;

FIG. 2 shows the longitudinal aberration of the camera optical lensshown in FIG. 1;

FIG. 3 shows the lateral color of the camera optical lens shown in FIG.1;

FIG. 4 shows a schematic diagram of the field curvature and distortionof the camera optical lens shown in FIG. 1;

FIG. 5 is a schematic diagram of a camera optical lens in accordancewith a second embodiment of the present invention;

FIG. 6 shows the longitudinal aberration of the camera optical lensshown in FIG. 5;

FIG. 7 shows the lateral color of the camera optical lens shown in FIG.5;

FIG. 8 shows the field curvature and distortion of the camera opticallens shown in FIG. 5:

FIG. 9 is a schematic diagram of a camera optical lens in accordancewith a third embodiment of the present invention;

FIG. 10 shows the longitudinal aberration of the camera optical lensshown in FIG. 9;

FIG. 11 shows the lateral color of the camera optical lens shown in FIG.9;

FIG. 12 shows the field curvature and distortion of the camera opticallens shown in FIG. 9.

DETAILED DESCRIPTION OF THE EXEMPLARY EMBODIMENTS

The present disclosure will hereinafter be described in detail withreference to several exemplary embodiments. To make the technicalproblems to be solved, technical solutions and beneficial effects of thepresent disclosure more apparent, the present disclosure is described infurther detail together with the figure and the embodiments. It shouldbe understood the specific embodiments described hereby is only toexplain the disclosure, not intended to limit the disclosure.

Embodiment 1

As referring to FIG. 1, the present invention provides a camera opticallens 10. FIG. 1 shows the camera optical lens 10 of embodiment 1 of thepresent invention, the camera optical lens 10 comprises 6 lenses.Specifically, from the object side to the image side, the camera opticallens 10 comprises in sequence: an aperture S1, a first lens L1, a secondlens L2, a third lens L3, a fourth lens L4, a fifth lens L5, and a sixthlens L6. Optical element like optical filter GF can be arranged betweenthe sixth lens L6 and the image surface Si.

The first lens L1 is made of plastic material, the second lens L2 ismade of plastic material, the third lens L3 is made of glass material,the fourth lens L4 is made of plastic material, the fifth lens L5 ismade of plastic material, and the sixth lens L6 is made of plasticmaterial.

In this embodiment, the second lens L2 has a negative refractive power.The third lens L3 has a negative refractive power.

Here, the focal length of the whole camera optical lens 10 is defined asf, the focal length of the first lens is defined as f1. The cameraoptical lens further satisfies the following condition: 0.1≤f1/f≤5,which fixes the positive refractive power of the first lens L1. If thelower limit of the set value is exceeded, although it benefits theultra-thin development of lenses, but the positive refractive power ofthe first lens L1 will be too strong, problem like aberration isdifficult to be corrected, and it is also unfavorable for wide-angledevelopment of lens. On the contrary, if the upper limit of the setvalue is exceeded, the positive refractive power of the first lens L1becomes too weak, it is then difficult to develop ultra-thin lenses.Preferably, the following condition shall be satisfied, 0.352≤f1/f≤4.74.

The refractive power of the third lens L3 is defined as n3. Here thefollowing condition should be satisfied: 1.7≤n3≤2.2. This conditionfixes the refractive power of the third lens L3, and when the value ofthe refractive power within this range benefits the ultra-thindevelopment of lenses, and it also benefits the correction ofaberration. Preferably, the following condition shall be satisfied,1.8≤n3≤2.08.

The thickness on-axis of the third lens L3 is defined as d5, and thetotal optical length of the camera optical lens 10 is defined as TTL.The following condition: 0.04≤d5/TTL≤0.1 should be satisfied. Thiscondition fixes the ratio between the thickness on-axis of the thirdlens L3 and the total optical length TTL. When the condition issatisfied, it is beneficial for realization of the ultra-thin lens.Preferably, the condition 0.045≤d5/TTL≤0.098 shall be satisfied.

When the focal length of the camera optical lens 10 of the presentinvention, the focal length of each lens, the refractive power of therelated lens, and the total optical length, the thickness on-axis andthe curvature radius of the camera optical lens satisfy the aboveconditions, the camera optical lens 10 has the advantage of highperformance and satisfies the design requirement of low TTL.

In this embodiment, the first lens L1 has a positive refractive powerwith a convex object side surface and a concave image side surfacerelative to the proximal axis.

The curvature radius of the object side surface of the first lens L1 isdefined as R1, the curvature radius of the image side surface of thefirst lens L1 is defined as R2. The camera optical lens 10 furthersatisfies the following condition: −16.89≤(R1+R2)/(R1−R2)≤−0.46, whichfixes the shape of the first lens L1, by which, the shape of the firstlens L1 can be reasonably controlled and it is effectively forcorrecting spherical aberration of the camera optical lens. Preferably,the condition −10.55≤(R1+R2)/(R1−R2)≤−0.57 shall be satisfied.

The thickness on-axis of the first lens L1 is defined as d1. Thefollowing condition: 0.13≤d1≤0.72 should be satisfied. When thecondition is satisfied, it is beneficial for realization of theultra-thin lens. Preferably, the condition 0.21≤d1≤0.58 shall besatisfied.

In this embodiment, the second lens L2 has a concave image side surfacerelative to the proximal axis.

The focal length of the whole camera optical lens 10 is f, the focallength of the second lens L2 is f2. The following condition should besatisfied: −2885.13≤f2/f≤−1.2. When the condition is satisfied, thenegative refractive power of the second lens L2 is controlled withinreasonable scope, the spherical aberration caused by the first lens L1which has positive refractive power and the field curvature of thesystem then can be reasonably and effectively balanced. Preferably, thecondition −1803.21≤f2/f≤−15 should be satisfied.

The curvature radius of the object side surface of the second lens L2 isdefined as R3, the curvature radius of the image side surface of thesecond lens L2 is defined as R4. The following condition should besatisfied: −0.53≤(R3+R4)/(R3−R4)≤72.75, which fixes the shape of thesecond lens L2, when the value is beyond this range, with thedevelopment into the direction of ultra-thin and wide-angle lenses,problem like aberration of the on-axis Chromatic aberration is difficultto be corrected. Preferably, the following condition shall be satisfied,−0.33≤(R3+R4)/(R3−R4)≤−58.2.

The thickness on-axis of the second lens L2 is defined as d3. Thefollowing condition: 0.11≤d3≤0.35 should be satisfied. When thecondition is satisfied, it is beneficial for realization of theultra-thin lens. Preferably, the condition 0.18≤d3≤0.28 shall besatisfied.

In this embodiment, the third lens L3 has a convex object side surfaceand a concave image side surface relative to the proximal axis.

The focal length of the whole camera optical lens 10 is f, the focallength of the third lens L3 is f3. The following condition should besatisfied: −6.8≤f3/f≤−1.37, by which the field curvature of the systemthen can be reasonably and effectively balanced. Preferably, thecondition −4.25≤f3/f≤−1.72 should be satisfied.

The curvature radius of the object side surface of the third lens L3 isdefined as R5, the curvature radius of the image side surface of thethird lens L3 is defined as R6. The following condition should besatisfied: 0.75≤(R5+R6)/(R5−R6)≤11.33, which is beneficial for theshaping of the third lens L3, and bad shaping and stress generation dueto extra-large curvature of surface of the third lens L3 can be avoided.Preferably, the following condition shall be satisfied,1.21≤(R5+R6)/(R5−R6)≤9.07.

The thickness on-axis of the third lens L3 is defined as d5. Thefollowing condition: 0.1≤d5≤0.6 should be satisfied. When the conditionis satisfied, it is beneficial for realization of the ultra-thin lens.Preferably, the condition 0.16≤d5≤0.48 shall be satisfied.

In this embodiment, the fourth lens L4 has a convex object side surfaceand a convex image side surface relative to the proximal axis.

The focal length of the whole camera optical lens 10 is f, the focallength of the fourth lens L4 is f4. The following condition should besatisfied: −19.68≤f4/f≤1.46, which can effectively reduce thesensitivity of lens group used in camera and further enhance the imagingquality. Preferably, the condition −12.3≤f4/f≤1.17 should be satisfied.

The curvature radius of the object side surface of the fourth lens L4 isdefined as R7, the curvature radius of the image side surface of thefourth lens L4 is defined as R8. The following condition should besatisfied: −3.61≤(R7+R8)/(R7−R8)≤13.36, which fixes the shaping of thefourth lens L4. When beyond this range, with the development into thedirection of ultra-thin and wide-angle lenses, problem like aberrationof the off-axis picture angle is difficult to be corrected. Preferably,the following condition shall be satisfied, −2.26≤(R7+R8)/(R7−R8)≤10.69.

The thickness on-axis of the fourth lens L4 is defined as d7. Thefollowing condition: 0.12≤d7≤0.58 should be satisfied. When thecondition is satisfied, it is beneficial for realization of theultra-thin lens. Preferably, the condition 0.18≤d7≤0.46 shall besatisfied.

In this embodiment, the fifth lens L5 has a positive refractive powerwith a convex image side surface relative to the proximal axis.

The focal length of the whole camera optical lens 10 is f, the focallength of the fifth lens L5 is f5. The following condition should besatisfied: 0.28≤f5/f≤1.67, which can effectively smooth the light anglesof the camera and reduce the tolerance sensitivity. Preferably, thecondition 0.45≤f5/f≤1.34 should be satisfied.

The curvature radius of the object side surface of the fifth lens L5 isto defined as R9, the curvature radius of the image side surface of thefifth lens L5 is defined as R10. The following condition should besatisfied: 0.43≤(R9+R10)/(R9−R10)≤2.23, by which, the shape of the fifthlens L5 is fixed, When beyond this range, with the development into thedirection of ultra-thin and wide-angle lenses, problem like aberrationof the off-axis picture angle is difficult to be corrected. Preferably,the following condition shall be satisfied, 0.69≤(R9+R10)/(R9−R10)≤1.78.

The thickness on-axis of the fifth lens L5 is defined as d9. Thefollowing condition: 0.17≤d9≤1.12 should be satisfied. When thecondition is satisfied, it is beneficial for realization of theultra-thin lens. Preferably, the condition 0.28≤d9≤0.9 shall besatisfied.

In this embodiment, the sixth lens L6 has a negative refractive powerwith a concave object side surface and a convex image side surfacerelative to the proximal axis.

The focal length of the whole camera optical lens 10 is f, the focallength of the sixth lens L6 is f6. The following condition should besatisfied: −1.43≤f6/f≤−0.25, which can effectively reduce thesensitivity of lens group used in camera and further enhance the imagingquality. Preferably, the condition −0.89≤f6/f≤−0.31 should be satisfied.

The curvature radius of the object side surface of the sixth lens L6 isdefined as R11, the curvature radius of the image side surface of thesixth lens L6 is defined as R12. The following condition should besatisfied: −1.47≤(R11+R12)/(R11−R12)≤0.78, by which, the shape of thesixth lens L6 is fixed, When beyond this range, with the developmentinto the direction of ultra-thin and wide-angle lenses, problem likeaberration of the off-axis picture angle is difficult to be corrected.Preferably, the following condition shall be satisfied,−0.92≤(R11+R12)/(R11−R12)≤0.62.

The thickness on-axis of the sixth lens L6 is defined as d11. Thefollowing condition: 0.11≤d11≤0.35 should be satisfied. When thecondition is satisfied, it is beneficial for realization of theultra-thin lens. Preferably, the condition 0.17≤d11≤0.28 shall besatisfied.

The focal length of the whole camera optical lens 10 is f, the combinedfocal length of the first lens L1 and the second lens L2 is f12. Thefollowing condition should be satisfied: 0.45≤f12/f≤6.47, which caneffectively avoid the aberration and field curvature of the cameraoptical lens, and can suppress the rear focal length for realizing theultra-thin lens. Preferably, the condition 0.63≤f12/f≤5.18 should besatisfied.

In this embodiment, the total optical length TTL of the camera opticallens 10 is less than or equal to 4.9 mm, it is beneficial for therealization of ultra-thin lenses. Preferably, the total optical lengthTTL of the camera optical lens 10 is less than or equal to 4.68 mm.

In this embodiment, the aperture F number of the camera optical lens isless than or equal to 2.27. A large aperture has better imagingperformance. Preferably, the aperture F number of the camera opticallens 10 is less than or equal to 2.22.

With such design, the total optical length TTL of the whole cameraoptical lens 10 can be made as short as possible, thus theminiaturization characteristics can be maintained.

In the following, an example will be used to describe the camera opticallens 10 of the present invention. The symbols recorded in each exampleare as follows. The unit of distance, radius and center thickness is mm.

TTL: Optical length (the distance on-axis from the object side surfaceof the first lens L1 to the image surface).

Preferably, inflexion points and/or arrest points can also be arrangedon the object side surface and/or image side surface of the lens, sothat the demand for high quality imaging can be satisfied, thedescription below can be referred for specific implementable scheme.

The design information of the camera optical lens 10 in the firstembodiment of the present invention is shown in the following, the unitof the focal length, distance, radius and center thickness is mm.

The design information of the camera optical lens 10 in the firstembodiment of the present invention is shown in the tables 1 and 2.

TABLE 1 R d nd v d S1 ∞ d0= −0.080 R1 1.3883 d1= 0.480 nd1 1.5441 v 156.04 R2 −7.5166 d2= 0.030 R3 −5.6697 43= 0.230 nd2 1.5441 v 2 56.04 R49.7457 d4= 0.086 R5 46.6580 d5= 0.200 nd3 1.9591 v 3 17.47 R6 9.4801 d6=0.342 R7 8.9373 d7= 0.243 nd4 1.6713 v 4 19.24 R8 6.4528 d8= 0.331 R920.6231 d9= 0.712 nd5 1.5441 v 5 56.04 R10 −1.1495 d10= 0.325 R11−0.8366 d11= 0.216 nd6 1.5352 v 6 56.09 R12 5.4227 d12= 0.121 R15 ∞ d13=0.210 ndg 1.5168 v g 64.17 R16 ∞ d14= 0.500

Where:

In which, the meaning of the various symbols is as follows.

S1: Aperture;

R: The curvature radius of the optical surface, the central curvatureradius in case of lens;

R1: The curvature radius of the object side surface of the first lensL1;

R2: The curvature radius of the image side surface of the first lens L1;

R3: The curvature radius of the object side surface of the second lensL2;

R4: The curvature radius of the image side surface of the second lensL2;

R5: The curvature radius of the object side surface of the third lensL3;

R6: The curvature radius of the image side surface of the third lens L3;

R7: The curvature radius of the object side surface of the fourth lensL4;

R8: The curvature radius of the image side surface of the fourth lensL4;

R9: The curvature radius of the object side surface of the fifth lensL5;

R10: The curvature radius of the image side surface of the fifth lensL5;

R11: The curvature radius of the object side surface of the sixth lensL6;

R12: The curvature radius of the image side surface of the sixth lensL6;

R13: The curvature radius of the object side surface of the opticalfilter GF;

R14: The curvature radius of the image side surface of the opticalfilter GF;

d: The thickness on-axis of the lens and the distance on-axis betweenthe lens;

d0: The distance on-axis from aperture S1 to the object side surface ofthe first lens L1;

d1: The thickness on-axis of the first lens L1;

d2: The distance on-axis from the image side surface of the first lensL1 to the object side surface of the second lens L2;

d3: The thickness on-axis of the second lens L2;

d4: The distance on-axis from the image side surface of the second lensL2 to the object side surface of the third lens L3;

d5: The thickness on-axis of the third lens L3;

d6: The distance on-axis from the image side surface of the third lensL3 to the object side surface of the fourth lens L4;

d7: The thickness on-axis of the fourth lens L4;

d8: The distance on-axis from the image side surface of the fourth lensL4 to the object side surface of the fifth lens L5;

d9: The thickness on-axis of the fifth lens L5;

d10: The distance on-axis from the image side surface of the fifth lensL5 to the object side surface of the sixth lens L6;

d11: The thickness on-axis of the sixth lens L6;

d12: The distance on-axis from the image side surface of the sixth lensL6 to the object side surface of the optical filter GF;

d13: The thickness on-axis of the optical filter GF;

d14: The distance on-axis from the image side surface to the imagesurface of the optical filter GF;

nd: The refractive power of the d line;

nd1: The refractive power of the d line of the first lens L1;

nd2: The refractive power of the d line of the second lens L2;

nd3: The refractive power of the d line of the third lens L3;

nd4: The refractive power of the d line of the fourth lens L4;

nd5: The refractive power of the d line of the fifth lens L5;

nd6: The refractive power of the d line of the sixth lens L6;

ndg: The refractive power of the d line of the optical filter GF;

vd: The abbe number;

v1: The abbe number of the first lens L1;

v2: The abbe number of the second lens L2;

v3: The abbe number of the third lens L3;

v4: The abbe number of the fourth lens L4;

v5: The abbe number of the fifth lens L5;

v6: The abbe number of the sixth lens L6;

vg: The abbe number of the optical filter GF.

Table 2 shows the aspherical surface data of the camera optical lens 10in the embodiment 1 of the present invention.

TABLE 2 Conic Index Aspherical Surface Index k A4 A6 A8 A10 A12 A14 A16R1 −1.6647E−01 −2.0524E−02 −2.6453E−02  −4.9003E−02 −2.7366E−02−5.3292E−02 −3.4305E−02   9.1869E−02 R2 −1.0811E+02 −9.1353E−039.0300E−03 −6.9621E−03 −4.2802E−02 −5.2572E−02 3.8741E−02  1.1710E−01 R3−1.0269E+02  3.8892E−02 5.1407E−02 −4.0114E−03 −3.3905E−02 −1.3000E−021.6774E−02 −1.4199E−02 R4 −2.4544E+01 −4.1979E−02 −9.4354E−02 −2.0831E−02 −3.0985E−02 −6.5138E−03 1.0772E−02  1.7120E−04 R5−9.7740E+01 −1.2821E−02 5.7287E−02 −8.6485E−03  4.4595E−02  5.1374E−02−4.3445E−03  −3.2418E−02 R6  7.1613E+01  5.3333E−02 8.7871E−02 7.2954E−02  2.5404E−03  3.4245E−03 4.6739E−02  1.8034E−01 R7 3.5677E+01 −2.1063E−01 9.5853E−02 −1.1105E−01 −4.3198E−02  1.0396E−011.2080E−01 −2.1055E−01 R8  2.5880E+01 −2.1014E−01 3.8288E−02 −8.6168E−03−1.2185E−02  9.8259E−03 3.1443E−02 −2.0667E−02 R9  9.9251E+01−3.4745E−02 −6.0523E−02   1.5670E−02 −9.5638E−03 −9.5690E−04 5.4176E−03−1.3496E−03 R10 −5.3339E+00 −1.1189E−02 2.0584E−02 −1.6510E−02 3.1705E−03  6.6411E−04 −5.2690E−04   8.2797E−05 R11 −4.2273E+00−5.5389E−02 1.2238E−02  6.1486E−04 −1.3838E−05  1.1453E−06 −8.1453E−07 −1.8359E−06 R12 −1.0429E+02 −3.0277E−02 3.9167E−03 −1.7968E−03−1.2672E−05 −2.5212E−05 2.0942E−05 −1.9430E−06

Among them, K is a conic index, A4, A6, A8, A10, A12, A14, A16 areaspheric surface indexes.

IH: Image height

y=(x ² /R)/[1+{1−(k+1)(x ² /R ²)}^(1/2)]+A4x ⁴ +A6x ⁶ +A8x ⁸ +A10x ¹⁰+A12x ¹² +A14x ¹⁴ +A16x ¹⁶  (1)

For convenience, the aspheric surface of each lens surface uses theaspheric surfaces shown in the above condition (1). However, the presentinvention is not limited to the aspherical polynomials form shown in thecondition (1).

Table 3 and table 4 show the inflexion points and the arrest pointdesign data of the camera optical lens 10 lens in embodiment 1 of thepresent invention. In which, P1R1 and P1R2 represent respectively theobject side surface and image side surface of the first lens L1, P2R1and P2R2 represent respectively the object side surface and image sidesurface of the second lens L2, P3R1 and P3R2 represent respectively theobject side surface and image side surface of the third lens L3, P4R1and P4R2 represent respectively the object side surface and image sidesurface of the fourth lens L4, P5R1 and P5R2 represent respectively theobject side surface and image side surface of the fifth lens L5, P6R1and P6R2 represent respectively the object side surface and image sidesurface of the sixth lens L6. The data in the column named “inflexionpoint position” are the vertical distances from the inflexion pointsarranged on each lens surface to the optic axis of the camera opticallens 10. The data in the column named “arrest point position” are thevertical distances from the arrest points arranged on each lens surfaceto the optic axis of the camera optical lens 10.

TABLE 3 Inflexion point Inflexion point Inflexion point number position1 position 2 P1R1 1 0.725 P1R2 1 0.785 P2R1 2 0.385 0.845 P2R2 1 0.345P3R1 0 P3R2 0 P4R1 1 0.225 P4R2 1 0.265 P5R1 2 0.305 1.305 P5R2 0 P6R1 21.295 1.905 P6R2 2 0.475 2.195

TABLE 4 Arrest point Arrest point number Arrest point position 1position 2 P1R1 0 P1R2 0 P2R1 1 0.665 P2R2 1 0.535 P3R1 0 P3R2 0 P4R1 0P4R2 1 0.455 P5R1 1 0.475 P5R2 0 P6R1 0 P6R2 1 0.915

FIG. 2 and FIG. 3 show the longitudinal aberration and lateral colorschematic diagrams after light with a wavelength of 470 nm, 555 nm and650 nm passes the camera optical lens 10 in the first embodiment. FIG. 4shows the field curvature and distortion schematic diagrams after lightwith a wavelength of 555 nm passes the camera optical lens 10 in thefirst embodiment, the field curvature S in FIG. 4 is a field curvaturein the sagittal direction, T is a field curvature in the meridiandirection.

Table 13 shows the various values of the embodiments 1, 2, 3, and thevalues corresponding with the parameters which are already specified inthe conditions.

As shown in Table 13, the first embodiment satisfies the variousconditions.

In this embodiment, the pupil entering diameter of the camera opticallens is 1.652 mm, the full vision field image height is 2.994 mm, thevision field angle in the diagonal direction is 79.25°, it haswide-angle and is ultra-thin, its on-axis and off-axis chromaticaberrations are fully corrected, and it has excellent opticalcharacteristics.

Embodiment 2

Embodiment 2 is basically the same as embodiment 1, the meaning of itssymbols is the same as that of embodiment 1, in the following, only thedifferences are described.

Table 5 and table 6 show the design data of the camera optical lens inembodiment 2 of the present invention.

TABLE 5 R d nd v d S1 ∞ d0= −0.080 R1 1.3938 d1= 0.407 nd1 1.5441 v 156.04 R2 10.9419 d2= 0.032 R3 11.8467 d3= 0.222 nd2 1.5441 v 2 56.04 R410.6498 d4= 0.068 R5 16.9076 d5= 0.400 nd3 1.8929 v 3 20.36 R6 4.7804d6= 0.327 R7 4.8488 d7= 0.231 nd4 1.6713 v 4 19.24 R8 3.8701 d8= 0.311R9 16.8177 d9= 0.749 nd5 1.5441 v 5 56.04 R10 −1.2030 d10= 0.320 R11−1.0848 d11= 0.230 nd6 1.5352 v 6 56.09 R12 3.5271 d12= 0.147 R15 ∞ d13=0.210 ndg 1.5168 v g 64.17 R16 ∞ d14= 0.500

Table 6 shows the aspherical surface data of each lens of the cameraoptical lens 20 in embodiment 2 of the present invention.

TABLE 6 Conic index Aspherical Surface Index k A4 A6 A8 A10 A12 A14 A16R1 −1.7941E−01 −1.7362E−02 −1.9833E−02  −3.3166E−02 −1.1474E−02−5.3392E−02 −5.1256E−02   4.9245E−02 R2  1.5753E+01 −5.5931E−023.1532E−03 −1.8682E−02 −4.8946E−02 −5.2864E−02 2.7992E−02  4.6430E−02 R3 7.0952E+01 −2.4558E−02 5.4106E−03 −1.6613E−02 −4.2270E−02 −2.8031E−023.6467E−03 −5.1654E−03 R4 −6.4194E+01 −4.1256E−02 −7.2225E−02 −1.2815E−02 −2.5897E−02 −3.0563E−03 1.9422E−04 −1.8888E−03 R5−4.4843E+01 −1.7842E−02 3.2610E−02 −1.7258E−02  4.0570E−02  5.1575E−02−9.5389E−03  −1.9668E−02 R6  1.2655E+01  1.2956E−02 7.3403E−02 5.8581E−02 −1.9019E−02 −1.3471E−02 2.8774E−02  1.8716E−01 R7−6.3657E+01 −2.0427E−01 7.1581E−02 −7.7776E−02 −2.8087E−02  6.6006E−026.9383E−02 −1.4333E−01 R8 −3.0142E+01 −1.9478E−01 4.9098E−02 −8.5166E−03−1.4778E−02  7.4766E−03 3.1561E−02 −1.9372E−02 R9  9.5101E+01−3.2039E−02 −4.9009E−02   1.8292E−02 −8.6606E−03 −8.3218E−04 5.1393E−03−1.5471E−03 R10 −5.5421E+00  2.1844E−03 1.6839E−02 −1.6525E−02 3.2619E−03  6.7888E−04 −5.1522E−04   7.9942E−05 R11 −6.1562E+00−6.5130E−02 1.0826E−02  4.9750E−04 −1.1962E−07  5.7469E−06 1.1178E−06−1.0703E−06 R12 −4.5436E+01 −3.4555E−02 2.2092E−03 −1.0234E−03 4.2888E−05 −4.6959E−05 1.9400E−05 −1.6638E−06

Table 7 and table 8 show the inflexion points and the arrest pointdesign data of the camera optical lens 20 lens in embodiment 2 of thepresent invention.

TABLE 7 Inflexion point Inflexion point Inflexion point number position1 position 2 P1R1 1 0.735 P1R2 1 0.375 P2R1 1 0.515 P2R2 1 0.345 P3R1 0P3R2 0 P4R1 1 0.265 P4R2 1 0.305 P5R1 1 0.345 P5R2 0 P6R1 1 1.445 P6R2 10.515

TABLE 8 Arrest point Arrest point Arrest point number position 1position 2 P1R1 0 P1R2 1 0.595 P2R1 1 0.715 P2R2 1 0.535 P3R1 0 P3R2 0P4R1 1 0.465 P4R2 1 0.545 P5R1 1 0.555 P5R2 0 P6R1 0 P6R2 1 0.995

FIG. 6 and FIG. 7 show the longitudinal aberration and lateral colorschematic diagrams after light with a wavelength of 470 nm, 555 nm and650 nm passes the camera optical lens 20 in the second embodiment. FIG.8 shows the field curvature and distortion schematic diagrams afterlight with a wavelength of 555 nm passes the camera optical lens 20 inthe second embodiment.

As shown in Table 13, the second embodiment satisfies the variousconditions.

In this embodiment, the pupil entering diameter of the camera opticallens is 1.6603 mm, the full vision field image height is 2.994 mm, thevision field angle in the diagonal direction is 77.910, it haswide-angle and is ultra-thin, its on-axis and off-axis chromaticaberrations are fully corrected, and it has excellent opticalcharacteristics.

Embodiment 3

Embodiment 3 is basically the same as embodiment 1, the meaning of itssymbols is the same as that of embodiment 1, in the following, only thedifferences are described.

Table 9 and table 10 show the design data of the camera optical lens inembodiment 3 of the present invention.

TABLE 9 R d nd v d S1 ∞ d0= −0.075 R1 2.2364 d1= 0.266 nd1 1.5352 v 156.09 R2 2.8373 d2= 0.074 R3 2.0219 d3= 0.230 nd2 1.5352 v 2 56.09 R41.9402 d4= 0.097 R5 2.1869 d5= 0.229 nd3 1.9591 v 3 17.47 R6 1.6756 d6=0.076 R7 1.4712 d7= 0.385 nd4 1.5352 v 4 56.09 R8 5.1282 d8= 0.565 R9−9.5085 d9= 0.347 nd5 1.5352 v 5 56.09 R10 −1.8596 d10= 1.093 R11−6.1130 d11= 0.230 nd6 1.5352 v 6 56.09 R12 1.9400 d12= 0.152 R15 ∞ d13=0.210 ndg 1.5168 v g 64.17 R16 ∞ d14= 0.500

Table 10 shows the aspherical surface data of each lens of the cameraoptical lens 30 in embodiment 3 of the present invention.

TABLE 10 Conic Index Aspherical Surface Index k A4 A6 A8 A10 A12 A14 A16R1 5.5956E−01 −2.3081E−02 −1.4402E−02   1.3019E−01 −1.1112E−01  3.7801E−02 −1.6318E−02 −1.2842E−02 R2 3.0956E+00 −1.0322E−01 2.1080E−02 1.5063E−01 −1.4623E−01  −7.7946E−02 −1.9717E−01  1.3174E−01 R39.2577E−01 −6.5238E−02 −8.4880E−02   1.4076E−01 −1.8200E−01  −2.8361E−01−6.5967E−02  1.5091E−01 R4 1.1077E+00 −1.1714E−01 −9.4901E−02 −1.9513E−01 5.7197E−02 −1.0609E−01  4.5776E−02  3.7897E−01 R5−2.0615E+00  −2.4750E−01 5.3927E−03 −1.4242E−01 2.2555E−02  1.6890E−01 1.8765E−01 −2.1681E−01 R6 −1.4112E+00  −2.9840E−01 9.9950E−02−3.7897E−02 1.4817E−02 −1.4390E−02 −2.0116E−02 −1.4984E−02 R7−3.6173E+00   9.2852E−03 1.5300E−01 −3.7801E−01 1.1021E+00 −1.7820E+00 1.4319E+00 −4.7233E−01 R8 1.9729E+01  1.2379E−02 7.0266E−03 −3 3135E−021.1658E−01  3.3062E−02 −1.4468E−01  2.7587E−02 R9 1.4381E+01  1.3930E−04−6.7903E−02   5.6804E−02 −9.8105E−02   1.5402E−01 −1.4499E−01 4.0692E−02 R10 −6.1091E−01   5.7928E−02 −3.4556E−02   2.8793E−025.1495E−02 −5.8391E−02  2.4734E−02 −4.4590E−03 R11 4.8091E+00−3.3575E−01 2.0541E−01 −5.9963E−02 1.1611E−02 −1.6366E−03  1.4259E−04−4.7450E−06 R12 −1.3919E+01  −1.6620E−01 7.7737E−02 −2.6162E−026.2824E−03 −1.0480E−03  1.0547E−04 −4.6667E−06

Table 11 and table 12 show the inflexion points and the arrest pointdesign data of the camera optical lens 30 lens in embodiment 3 of thepresent invention.

TABLE 11 Inflexion point Inflexion point Inflexion point number position1 position 2 P1R1 0 P1R2 1 0.665 P2R1 1 0.585 P2R2 2 0.495 0.805 P3R1 10.385 P3R2 1 0.435 P4R1 1 0.925 P4R2 1 0.915 P5R1 0 P5R2 1 0.785 P6R1 11.185 P6R2 1 0.405

TABLE 12 Arrest point Arrest point Arrest point number position 1position 2 P1R1 0 P1R2 1 0.825 P2R1 1 0.775 P2R2 2 0.765 0.825 P3R1 10.635 P3R2 1 0.765 P4R1 0 P4R2 0 P5R1 0 P5R2 1 1.165 P6R1 0 P6R2 1 0.815

FIG. 10 and FIG. 11 show the longitudinal aberration and lateral colorschematic diagrams after light with a wavelength of 470 nm, 555 nm and650 nm passes the camera optical lens 30 in the third embodiment. FIG.12 shows the field curvature and distortion schematic diagrams afterlight with a wavelength of 555 nm passes the camera optical lens 30 inthe third embodiment.

As shown in Table 13, the third embodiment satisfies the variousconditions.

In this embodiment, the pupil entering diameter of the camera opticallens is 1.727 mm, the full vision field image height is 2.994 mm, thevision field angle in the diagonal direction is 76.93°, it haswide-angle and is ultra-thin, its on-axis and off-axis chromaticaberrations are fully corrected, and it has excellent opticalcharacteristics.

TABLE 13 Embodiment Embodiment Embodiment 1 2 3 f 3.624 3.653 3.799 f12.189 2.883 17.029 f2 −6.532 −206.656 −5480.979 f3 −12.313 −7.517 −9.490f4 −35.664 −31.280 3.706 f5 2.018 2.087 4.238 f6 −1.334 1.519 −2.716 f123.045 2.897 16.398 (R1 + R2)/(R1 − R2) −0.688 −1.292 −8.444 (R3 +R4)/(R3 − R4) −0.264 18.796 48.503 (R5 + R6)/(R5 − R6) 1.510 1.788 7.555(R7 + R8)/(R7 − R8) 6.195 8.909 −1.805 (R9 + R10)/(R9 − R10) 0.894 0.8661.486 (R11 + R12)/(R11 − R12) −0.733 −0.530 0.518 f1/f 0.604 0.789 4.482f2/f −1.803 56.578 −1442.565 f3/f −3.398 −2.058 −2.498 f4/f −9.842−8.564 0.975 f5/f 0.557 0.571 1.115 f6/f −0.368 −0.416 −0.715 f12/f0.840 0.793 4.316 d1 0.480 0.407 0.266 d3 0.230 0.222 0.230 d5 0.2000.400 0.229 d7 0.243 0.231 0.385 d9 0.712 0.749 0.347 d11 0.216 0.2300.230 Fno 2.194 2.200 2.200 TTL 4.026 4.153 4.454 d1/TTL 0.119 0.0980.060 d3/TTL 0.057 0.053 0.052 d5/TTL 0.050 0.096 0.051 d7/TTL 0.0600.056 0.086 d9/TTL 0.177 0.180 0.078 d11/TTL 0.054 0.055 0.052 n1 1.54411.5441 1.5352 n2 1.5441 1.5441 1.5352 n3 1.9591 1.8929 1.9591 n4 1.67131.6713 1.5352 n5 1.5441 1.5441 1.5352 n6 1.5352 1.5352 1.5352 v1 56.037956.0379 56.0934 v2 56.0379 56.0379 56.0934 v3 17.4713 20.3618 17.4713 v419.2429 19.2429 56.0934 v5 56.0379 56.0379 56.0934 v6 56.0934 56.093456.0934

It is to be understood, however, that even though numerouscharacteristics and advantages of the present exemplary embodiments havebeen set forth in the foregoing description, together with details ofthe structures and functions of the embodiments, the disclosure isillustrative only, and changes may be made in detail, especially inmatters of shape, size, and arrangement of parts within the principlesof the invention to the full extent indicated by the broad generalmeaning of the terms where the appended claims are expressed.

What is claimed is:
 1. A camera optical lens comprising, from an objectside to an image side in sequence: a first lens, a second lens having anegative refractive power, a third lens having a positive refractivepower, a fourth lens, a fifth lens, and a sixth lens; wherein the cameraoptical lens further satisfies the following conditions:0.1≤f1/f≤5;1.7≤n3≤2.2;0.04≤d5/TTL≤0.1; where f: the focal length of the camera optical lens;f1: the focal length of the first lens; n3: the refractive power of thethird lens; d5: the thickness on-axis of the third lens; TTL: the totaloptical length of the camera optical lens.
 2. The camera optical lens asdescribed in claim 1, wherein the first lens is made of plasticmaterial, the second lens is made of plastic material, the third lens ismade of glass material, the fourth lens is made of plastic material, thefifth lens is made of plastic material, the sixth lens is made ofplastic material.
 3. The camera optical lens as described in claim 1further satisfying the following conditions:0.352≤f1/f≤4.74;1.8≤n3≤2.08;0.045≤d5/TTL≤0.098.
 4. The camera optical lens as described in claim 1,wherein first lens has a positive refractive power with a convex objectside surface relative to the proximal axis; the camera optical lensfurther satisfies the following conditions:−16.89≤(R1+R2)/(R1−R2)≤−0.46;0.13≤d1≤0.72; where R1: the curvature radius of object side surface ofthe first lens; R2: the curvature radius of image side surface of thefirst lens. d1: the thickness on-axis of the first lens.
 5. The cameraoptical lens as described in claim 4 further satisfying the followingconditions:−10.55≤(R1+R2)/(R1−R2)≤−0.57;0.21≤d1≤0.58.
 6. The camera optical lens as described in claim 1,wherein the second lens has a concave image side surface relative to theproximal axis; the camera optical lens further satisfies the followingconditions:−2885.13≤f2/f≤−1.2;−0.53≤(R3+R4)/(R3−R4)≤72.75;0.11≤d3≤0.35; where: f: the focal length of the camera optical lens; f2:the focal length of the second lens; R3: the curvature radius of theobject side surface of the second lens; R4: the curvature radius of theimage side surface of the second lens; d3: the thickness on-axis of thesecond lens.
 7. The camera optical lens as described in claim 6 furthersatisfying the following conditions:−1803.21≤f2/f≤−1.5;−0.33≤(R3+R4)/(R3−R4)≤58.2;0.18≤d3≤0.28.
 8. The camera optical lens as described in claim 1,wherein the third lens has a convex object side surface and a concaveimage side surface relative to the proximal axis; the camera opticallens further satisfies the following conditions:−6.8≤f3/f≤−1.37;0.75≤(R5+R6)/(R5−R6)≤11.33;0.1≤d5≤0.6; where f: the focal length of the camera optical lens; f3:the focal length of the third lens; R5: the curvature radius of theobject side surface of the third lens; R6: the curvature radius of theimage side surface of the third lens; d5: the thickness on-axis of thethird lens.
 9. The camera optical lens as described in claim 8 furthersatisfying the following conditions:−4.25≤f3/f≤−1.72;1.21≤(R5+R6)/(R5−R6)≤9.07;0.16≤d5≤0.48.
 10. The camera optical lens as described in claim 1,wherein the fourth lens has a convex object side surface and a conveximage side surface relative to the proximal axis; the camera opticallens further satisfies the following to conditions:−19.68≤f4/f≤1.46;−3.61≤(R7+R8)/(R7−R8)≤13.36;0.12≤d7≤0.58; where f: the focal length of the camera optical lens; f4:the focal length of the fourth lens; R7: the curvature radius of theobject side surface of the fourth lens; R8: the curvature radius of theimage side surface of the fourth lens; d7: the thickness on-axis of thefourth lens.
 11. The camera optical lens as described in claim 10further satisfying the following conditions:−12.3≤f4/f≤1.17;−2.26≤(R7+R8)/(R7−R8)≤10.69;0.18≤d7≤0.46.
 12. The camera optical lens as described in claim 1,wherein the fifth lens has a positive refractive power with a conveximage side surface relative to the proximal axis; the camera opticallens further satisfies the following conditions:0.28≤f5/f≤1.67;0.43≤(R9+R10)/(R9−R10)≤2.23;0.17≤d9≤1.12; where f: the focal length of the camera optical lens; f5:the focal length of the fifth lens; R9: the curvature radius of theobject side surface of the fifth lens; R10: the curvature radius of theimage side surface of the fifth lens; d9: the thickness on-axis of thefifth lens.
 13. The camera optical lens as described in claim 12 furthersatisfying the following conditions:0.45≤f5/f≤1.34;0.69≤(R9+R10)/(R9−R10)≤1.78;0.28≤d9≤0.9.
 14. The camera optical lens as described in claim 1,wherein the sixth lens has a negative refractive power with a concaveobject side surface and a convex image side surface; the camera opticallens further satisfies the following conditions:−1.43≤f6/f≤−0.25;−1.47≤(R11+R12)/(R11−R12)≤0.78;0.11≤d11≤0.35; where f: the focal length of the camera optical lens; f6:the focal length of the sixth lens; R11: the curvature radius of theobject side surface of the sixth lens; R12: the curvature radius of theimage side surface of the sixth lens; d11: the thickness on-axis of thesixth lens.
 15. The camera optical lens as described in claim 14 furthersatisfying the following conditions:−0.89≤f6/f≤−0.31;−0.92≤(R11+R12)/(R11−R12)≤0.62;0.17≤d11≤0.28.
 16. The camera optical lens as described in claim 1further satisfying the following condition:0.4≤f12/f≤6.47; where f12: the combined focal length of the first lensand the second lens; f: the focal length of the camera optical lens. 17.The camera optical lens as described in claim 16 further satisfying thefollowing condition:0.63≤f12/f≤5.18.
 18. The camera optical lens as described in claim 1,wherein the total optical length TTL of the camera optical lens is lessthan or equal to 4.9 mm.
 19. The camera optical lens as described inclaim 18, wherein the total optical length TTL of the camera opticallens is less than or equal to 4.68 mm.
 20. The camera optical lens asdescribed in claim 1, wherein the aperture F number of the cameraoptical lens is less than or equal to 2.27.
 21. The camera optical lensas described in claim 20, wherein the aperture F number of the cameraoptical lens is less than or equal to 2.22.